In chaos theory, the problem anti-synchronization of chaotic systems deals with a pair of chaotic systems
called drive and response systems. In this problem, the design goal is to drive the sum of their respective
states to zero asymptotically. This problem gets even more complicated and requires special attention when
the parameters of the drive and response systems are unknown. This paper uses adaptive control theory
and Lyapunov stability theory to derive new results for the anti-synchronization of hyperchaotic Wang
system (2008) and hyperchaotic Li system (2005) with uncertain parameters. Hyperchaotic systems are
nonlinear dynamical systems exhibiting chaotic behaviour with two or more positive Lyapunov exponents.
The hyperchaotic systems have applications in areas like oscillators, lasers, neural networks, encryption,
secure transmission and secure communication. The main results derived in this paper are validated and
demonstrated with MATLAB simulations.
ADAPTIVE CONTROLLER DESIGN FOR THE ANTI-SYNCHRONIZATION OF HYPERCHAOTIC YANG ...ijics
In the anti-synchronization of chaotic systems, a pair of chaotic systems called drive and responsesystems
are considered, and the design goal is to drive the sum of their respective states to zero asymptotically. This
paper derives new results for the anti-synchronization of hyperchaotic Yang system (2009) and
hyperchaotic Pang system (2011) with uncertain parameters via adaptive control. Hyperchaotic systems
are nonlinear chaotic systems withtwo or more positive Lyapunov exponents and they have applications in
areas like neural networks, encryption, secure data transmission and communication. The main results
derived in this paper are illustrated with MATLAB simulations.
ADAPTIVESYNCHRONIZER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC ZH...ijitcs
This paper derives new adaptive synchronizers for the hybrid synchronization of hyperchaotic Zheng
systems (2010) and hyperchaotic Yu systems (2012). In the hybrid synchronization design of master and
slave systems, one part of the systems, viz. their odd states, are completely synchronized (CS), while the
other part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the
process of synchronization. The research problem gets even more complicated, when the parameters of the
hyperchaotic systems are not known and we handle this complicate problem using adaptive control. The
main results of this research work are established via adaptive control theory andLyapunov stability
theory. MATLAB plotsusing classical fourth-order Runge-Kutta method have been depictedfor the new
adaptive hybrid synchronization results for the hyperchaotic Zheng and hyperchaotic Yu systems.
ADAPTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC XU ...ijait
This paper derives new adaptive results for the hybrid synchronization of hyperchaotic Xi systems (2009)
and hyperchaotic Li systems (2005). In the hybrid synchronization design of master and slave systems, one
part of the systems, viz. their odd states, are completely synchronized (CS), while the other part, viz. their
even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the process of
synchronization. The research problem gets even more complicated, when the parameters of the
hyperchaotic systems are unknown and we tackle this problem using adaptive control. The main results of
this research work are proved using adaptive control theory and Lyapunov stability theory. MATLAB
simulations using classical fourth-order Runge-Kutta method are shown for the new adaptive hybrid
synchronization results for the hyperchaotic Xu and hyperchaotic Li systems.
ACTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC XU AN...Zac Darcy
The synchronization of chaotic systems treats a pair of chaotic systems, which are usually called as master
and slave systems. In the chaos synchronization problem, the goal of the design is to synchronize the states
of master and slave systems asymptotically. In the hybrid synchronization design of master and slave
systems, one part of the systems, viz. their odd states, are completely synchronized (CS), while the other
part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the process
of synchronization. This research work deals with the hybrid synchronization of hyperchaotic Xi systems
(2009) and hyperchaotic Li systems (2005). The main results of this hybrid research work are established
with Lyapunov stability theory. MATLAB simulations of the hybrid synchronization results are shown for
the hyperchaotic Xu and Li systems.
ACTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC ZHEN...ijscai
This paper deals with a new research problem in the chaos literature, viz. hybrid synchronization of a
pair of chaotic systems called the master and slave systems. In the hybrid synchronization design of
master and slave systems, one part of the systems, viz. their odd states, are completely synchronized (CS),
while the other part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS coexist in the process of synchronization. This research work deals with the hybrid synchronization of
hyperchaotic Zheng systems (2010) and hyperchaotic Yu systems (2012). The main results of this hybrid
synchronization research work have been proved using Lyapunov stability theory. Numerical examples of
the hybrid synchronization results are shown along with MATLAB simulations for the hyperchaotic
Zheng and hyperchaotic Yu systems.
GLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN LORENZ-STENFLO AND QI 4-D CHAOTIC S...ijistjournal
In this paper, we apply adaptive control method to derive new results for the global chaos synchronization of 4-D chaotic systems, viz. identical Lorenz-Stenflo(LS) systems (Stenflo, 2001), identical Qi systems (Qi, Chen and Du, 2005) and non-identical LS and Qi systems. In this paper, we shall assume that the parameters of both master and slave systems are unknown and we devise adaptive control schemes for synchronization using the estimates of parameters for both master and slave systems. Our adaptive synchronization schemes derived in this paper are established using Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the adaptive control method is very effective and convenient to synchronize identical and non-identical LS and Qi systems.
Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive synchronization schemes for the identical and non-identical, uncertain LS and Qi 4-D chaotic systems.
ADAPTIVE CONTROL AND SYNCHRONIZATION OF SPROTT-I SYSTEM WITH UNKNOWN PARAMETERSijscai
This paper derives new results for the adaptive control and synchronization design of the Sprott-I chaotic system (1994), when the system parameters are unknown. First, we build an adaptive controller to stabilize the Sprott-I chaotic system to its unstable equilibrium at the origin. Then we build an adaptive
synchronizer to achieve global chaos synchronization of the identical Sprott-I chaotic systems with unknown parameters. The results derived for adaptive stabilization and adaptive synchronization for the Sprott-I chaotic system have been established using adaptive control theory and Lyapunov stability
theory. Numerical simulations have been shown to demonstrate the effectiveness of the adaptive control and synchronization schemes derived in this paper for the Sprott-I chaotic system.
ADAPTIVE CHAOS CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC LIU SYSTEM ijcseit
The hyperchaotic Liu system (Wang and Liu, 2006) is one of the important models of four-dimensional
hyperchaotic systems. This paper investigates the adaptive chaos control and synchronization of
hyperchaotic Liu system with unknown parameters. First, adaptive control laws are designed to stabilize
the hyperchaotic Liu system to its unstable equilibrium at the origin based on the adaptive control theory
and Lyapunov stability theory. Then adaptive control laws are derived to achieve global chaos
synchronization of identical hyperchaotic Liu systems with unknown parameters. Numerical simulations
are presented to demonstrate the effectiveness of the proposed adaptive chaos control and
synchronization schemes.
ADAPTIVE CONTROLLER DESIGN FOR THE ANTI-SYNCHRONIZATION OF HYPERCHAOTIC YANG ...ijics
In the anti-synchronization of chaotic systems, a pair of chaotic systems called drive and responsesystems
are considered, and the design goal is to drive the sum of their respective states to zero asymptotically. This
paper derives new results for the anti-synchronization of hyperchaotic Yang system (2009) and
hyperchaotic Pang system (2011) with uncertain parameters via adaptive control. Hyperchaotic systems
are nonlinear chaotic systems withtwo or more positive Lyapunov exponents and they have applications in
areas like neural networks, encryption, secure data transmission and communication. The main results
derived in this paper are illustrated with MATLAB simulations.
ADAPTIVESYNCHRONIZER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC ZH...ijitcs
This paper derives new adaptive synchronizers for the hybrid synchronization of hyperchaotic Zheng
systems (2010) and hyperchaotic Yu systems (2012). In the hybrid synchronization design of master and
slave systems, one part of the systems, viz. their odd states, are completely synchronized (CS), while the
other part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the
process of synchronization. The research problem gets even more complicated, when the parameters of the
hyperchaotic systems are not known and we handle this complicate problem using adaptive control. The
main results of this research work are established via adaptive control theory andLyapunov stability
theory. MATLAB plotsusing classical fourth-order Runge-Kutta method have been depictedfor the new
adaptive hybrid synchronization results for the hyperchaotic Zheng and hyperchaotic Yu systems.
ADAPTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC XU ...ijait
This paper derives new adaptive results for the hybrid synchronization of hyperchaotic Xi systems (2009)
and hyperchaotic Li systems (2005). In the hybrid synchronization design of master and slave systems, one
part of the systems, viz. their odd states, are completely synchronized (CS), while the other part, viz. their
even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the process of
synchronization. The research problem gets even more complicated, when the parameters of the
hyperchaotic systems are unknown and we tackle this problem using adaptive control. The main results of
this research work are proved using adaptive control theory and Lyapunov stability theory. MATLAB
simulations using classical fourth-order Runge-Kutta method are shown for the new adaptive hybrid
synchronization results for the hyperchaotic Xu and hyperchaotic Li systems.
ACTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC XU AN...Zac Darcy
The synchronization of chaotic systems treats a pair of chaotic systems, which are usually called as master
and slave systems. In the chaos synchronization problem, the goal of the design is to synchronize the states
of master and slave systems asymptotically. In the hybrid synchronization design of master and slave
systems, one part of the systems, viz. their odd states, are completely synchronized (CS), while the other
part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS co-exist in the process
of synchronization. This research work deals with the hybrid synchronization of hyperchaotic Xi systems
(2009) and hyperchaotic Li systems (2005). The main results of this hybrid research work are established
with Lyapunov stability theory. MATLAB simulations of the hybrid synchronization results are shown for
the hyperchaotic Xu and Li systems.
ACTIVE CONTROLLER DESIGN FOR THE HYBRID SYNCHRONIZATION OF HYPERCHAOTIC ZHEN...ijscai
This paper deals with a new research problem in the chaos literature, viz. hybrid synchronization of a
pair of chaotic systems called the master and slave systems. In the hybrid synchronization design of
master and slave systems, one part of the systems, viz. their odd states, are completely synchronized (CS),
while the other part, viz. their even states, are completely anti-synchronized (AS) so that CS and AS coexist in the process of synchronization. This research work deals with the hybrid synchronization of
hyperchaotic Zheng systems (2010) and hyperchaotic Yu systems (2012). The main results of this hybrid
synchronization research work have been proved using Lyapunov stability theory. Numerical examples of
the hybrid synchronization results are shown along with MATLAB simulations for the hyperchaotic
Zheng and hyperchaotic Yu systems.
GLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN LORENZ-STENFLO AND QI 4-D CHAOTIC S...ijistjournal
In this paper, we apply adaptive control method to derive new results for the global chaos synchronization of 4-D chaotic systems, viz. identical Lorenz-Stenflo(LS) systems (Stenflo, 2001), identical Qi systems (Qi, Chen and Du, 2005) and non-identical LS and Qi systems. In this paper, we shall assume that the parameters of both master and slave systems are unknown and we devise adaptive control schemes for synchronization using the estimates of parameters for both master and slave systems. Our adaptive synchronization schemes derived in this paper are established using Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the adaptive control method is very effective and convenient to synchronize identical and non-identical LS and Qi systems.
Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive synchronization schemes for the identical and non-identical, uncertain LS and Qi 4-D chaotic systems.
ADAPTIVE CONTROL AND SYNCHRONIZATION OF SPROTT-I SYSTEM WITH UNKNOWN PARAMETERSijscai
This paper derives new results for the adaptive control and synchronization design of the Sprott-I chaotic system (1994), when the system parameters are unknown. First, we build an adaptive controller to stabilize the Sprott-I chaotic system to its unstable equilibrium at the origin. Then we build an adaptive
synchronizer to achieve global chaos synchronization of the identical Sprott-I chaotic systems with unknown parameters. The results derived for adaptive stabilization and adaptive synchronization for the Sprott-I chaotic system have been established using adaptive control theory and Lyapunov stability
theory. Numerical simulations have been shown to demonstrate the effectiveness of the adaptive control and synchronization schemes derived in this paper for the Sprott-I chaotic system.
ADAPTIVE CHAOS CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC LIU SYSTEM ijcseit
The hyperchaotic Liu system (Wang and Liu, 2006) is one of the important models of four-dimensional
hyperchaotic systems. This paper investigates the adaptive chaos control and synchronization of
hyperchaotic Liu system with unknown parameters. First, adaptive control laws are designed to stabilize
the hyperchaotic Liu system to its unstable equilibrium at the origin based on the adaptive control theory
and Lyapunov stability theory. Then adaptive control laws are derived to achieve global chaos
synchronization of identical hyperchaotic Liu systems with unknown parameters. Numerical simulations
are presented to demonstrate the effectiveness of the proposed adaptive chaos control and
synchronization schemes.
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTORijcseit
This paper derives new results for the adaptive chaos stabilization and synchronization of Lü-like attractor
with unknown parameters. The Lü-like attractor is one of the recently discovered 3-scroll chaotic systems,
which was proposed by D. Li (2007). First, adaptive control laws are determined to stabilize the Lü-like
attractor to its unstable equilibrium at the origin. These adaptive laws are established using Lyapunov
stability theory. Then adaptive synchronization laws are determined so as to achieve global chaos
synchronization of identical Lü-like attractors with unknown parameters. Numerical simulations are
presented to validate and demonstrate the effectiveness of the proposed adaptive control and
synchronization schemes for the Lü-like attractor.
GLOBAL CHAOS SYNCHRONIZATION OF HYPERCHAOTIC QI AND HYPERCHAOTIC JHA SYSTEMS ...ijistjournal
This paper derives new results for the global chaos synchronization of identical hyperchaotic Qi systems (2008), identical hyperchaotic Jha systems (2007) and non-identical hyperchaotic Qi and Jha systems. Active nonlinear control is the method adopted to achieve the complete synchronization of the identical and different hyperchaotic Qi and Jha systems. Our stability results derived in this paper are established using Lyapunov stability theory. Numerical simulations are shown to validate and illustrate the effectiveness of the synchronization results derived in this paper.
THE DESIGN OF ADAPTIVE CONTROLLER AND SYNCHRONIZER FOR QI-CHEN SYSTEM WITH UN...IJCSEA Journal
This paper investigates the design problem of adaptive controller and synchronizer for the Qi-Chen system (2005), when the system parameters are unknown. First, we build an adaptive controller to stabilize the QiChen chaotic system to its unstable equilibrium at the origin. Then we build an adaptive synchronizer to achieve global chaos synchronization of the identical Qi-Chen chaotic systems with unknown parameters. The results derived for adaptive stabilization and adaptive synchronization for the Qi-Chen chaotic system are established using adaptive control theory and Lyapunov stability theory. Numerical simulations have been shown to demonstrate the effectiveness of the adaptive control and synchronization schemes derived in this paper for the Qi-Chen chaotic system.
ADAPTIVE CONTROL AND SYNCHRONIZATION OF LIU’S FOUR-WING CHAOTIC SYSTEM WITH C...IJCSEA Journal
This paper investigates the adaptive chaos control and synchronization of Liu’s four-wing chaotic system with cubic nonlinearity (Liu, 2009) and unknown parameters. First, we design adaptive control laws to stabilize the Liu’s four-wing chaotic system with cubic nonlinearity to its unstable equilibrium at the origin based on the adaptive control theory and Lyapunov stability theory. Next, we derive adaptive control laws to achieve global chaos synchronization of identical Liu’s four-wing chaotic systems with cubic nonlinearity and unknown parameters. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive chaos control and synchronization schemes.
Adaptive Controller Design For The Synchronization Of Moore-Spiegel And Act S...ijcsa
In this paper, we design adaptive controllers for the global chaos synchronization of identical MooreSpiegel systems (1966), identical ACT systems (1981) and non-identical Moore-Spiegel and ACT chaotic systems with unknown parameters. Our adaptive synchronization results derived in this paper for
uncertain Moore-Spiegel and ACT systems are established using Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the adaptive control method is very effective and convenient to synchronize identical and non-identical uncertain Moore-Spiegel and ACT chaotic
systems. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive synchronization schemes for the global chaos synchronization of the uncertain chaotic systems derived in this paper.
Adaptive Projective Lag Synchronization of T and Lu Chaotic Systems IJECEIAES
In this paper, the synchronization problem of T chaotic system and Lu chaotic system is studied. The parameter of the drive T chaotic system is considered unknown. An adaptive projective lag control method and also parameter estimation law are designed to achieve chaos synchronization problem between two chaotic systems. Then Lyapunov stability theorem is utilized to prove the validity of the proposed control method. After that, some numerical simulations are performed to assess the performance of the proposed method. The results show high accuracy of the proposed method in control and synchronization of chaotic systems.
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC BAO AND HYPERCHAOTIC XU SYSTEMS VIA ACTI...IJCSEIT Journal
This paper investigates the anti-synchronization of identical hyperchaotic Bao systems (Bao and Liu,
2008), identical hyperchaotic Xu systems (Xu, Cai and Zheng, 2009) and non-identical hyperchaotic Bao
and hyperchaotic Xu systems. Active nonlinear control has been deployed for the anti- synchronization of
the hyperchaotic systems addressed in this paper and the main results have been established using
Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the active
nonlinear control method is very effective and convenient to achieve anti-synchronization of identical and
non-identical hyperchaotic Bao and hyperchaotic Xu systems. Numerical simulations have been provided to
validate and demonstrate the effectiveness of the anti-synchronization results for the hyperchaotic Cao and
hyperchaotic Xu systems.
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...ijctcm
Hyperchaotic systems are chaotic systems having more than one positive Lyapunov exponent and they have
important applications in secure data transmission and communication. This paper applies active control
method for the synchronization of identical and different hyperchaotic Pang systems (2011) and
hyperchaotic Wang-Chen systems (2008). Main results are proved with the stability theorems of Lypuanov
stability theory and numerical simulations are plotted using MATLAB to show the synchronization of
hyperchaotic systems addressed in this paper.
ACTIVE CONTROLLER DESIGN FOR THE OUTPUT REGULATION OF THE WANG-CHEN-YUAN SYSTEMecij
In this paper, we design an active controller for regulating the output of the Wang-Chen-Yuan system (2009), which is one of the recently discovered 3-D chaotic systems. For the constant tracking problem, new state feedback control laws have been derived for regulating the output of the Wang-Chen-Yuan system. Numerical simulations using MATLAB are exhibited to validate and demonstrate the usefulness of the active controller design for the output regulation of the Wang-Chen-Yuan system.
STATE FEEDBACK CONTROLLER DESIGN FOR THE OUTPUT REGULATION OF SPROTT-H SYSTEMijistjournal
This paper investigates the problem of state feedback controller design for the output regulation of SprottK chaotic system, which is one of the simple, classical, three-dimensional chaotic systems discovered by J.C. Sprott (1994). Explicitly, we have derived new state feedback control laws for the constant tracking problem for the Sprott-H system. The state feedback control laws have been derived using the regulator equations of C.I. Byrnes and A. Isidori (1990). The output regulation of the Sprott H chaotic system has important applications in Electronics and Communication Engineering. Numerical simulations are shown to illustrate the effectiveness of the control schemes proposed in this paper for the output regulation of the Sprott-H chaotic system.
ANALYSIS AND SLIDING CONTROLLER DESIGN FOR HYBRID SYNCHRONIZATION OF HYPERCHA...IJCSEA Journal
Hybrid synchronization of chaotic systems is a research problem with a goal to synchronize the states of master and slave chaotic systems in a hybrid manner, namely, their even states are completely synchronized (CS) and odd states are anti-synchronized. This paper deals with the research problem of hybrid synchronization of chaotic systems. First, a detailed analysis is made on the qualitative properties of hyperchaotic Yujun system (2010). Then sliding controller has been derived for the hybrid synchronization of identical hyperchaotic Yujun systems, which is based on a general hybrid result derived in this paper.MATLAB simulations have been shown in detail to illustrate the new results derived for the hybrid synchronization of hyperchaotic Yujun systems. The results are proved using Lyapunov stability theory.
ADAPTIVE CONTROL AND SYNCHRONIZATION OF A HIGHLY CHAOTIC ATTRACTORijistjournal
Recently, a novel three-dimensional highly chaotic attractor has been discovered by Srisuchinwong and Munmuangsaen (2010). This paper investigates the adaptive control and synchronization of this highly chaotic attractor with unknown parameters. First, adaptive control laws are designed to stabilize the highly chaotic system to its unstable equilibrium point at the origin based on the adaptive control theory and Lyapunov stability theory. Then adaptive control laws are derived to achieve global chaos synchronization of identical highly chaotic systems with unknown parameters. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive control and synchronization schemes.
This paper presents synchronization of a new autonomous hyperchaotic system. The generalized
backstepping technique is applied to achieve hyperchaos synchronization for the two new hyperchaotic
systems. Generalized backstepping method is similarity to backstepping. Backstepping method is used only
to strictly feedback systems but generalized backstepping method expands this class. Numerical simulations
are presented to demonstrate the effectiveness of the synchronization schemes.
Projective and hybrid projective synchronization of 4-D hyperchaotic system v...TELKOMNIKA JOURNAL
Nonlinear control strategy was established to realize the Projective Synchronization (PS) and Hybrid Projective Synchronization (HPS) for 4-D hyperchaotic system at different scaling matrices. This strategy, which is able to achieve projective and hybrid projective synchronization by more precise and adaptable method to provide a novel control scheme. On First stage, three scaling matrices were given in order to achieving various projective synchronization phenomena. While the HPS was implemented at specific scaling matrix in the second stage. Ultimately, the precision of controllers were compared and analyzed theoretically and numerically. The long-range precision of the proposed controllers are confirmed by third stage.
Chaos synchronization in a 6-D hyperchaotic system with self-excited attractorTELKOMNIKA JOURNAL
This paper presented stability application for chaos synchronization using a 6-D hyperchaotic system of different controllers and two tools: Lyapunov stability theory and Linearization methods. Synchronization methods based on nonlinear control strategy is used. The selecting controller's methods have been modified by applying complete synchronization. The Linearization methods can achieve convergence according to the of complete synchronization. Numerical simulations are carried out by using MATLAB to validate the effectiveness of the analytical technique.
DYNAMICS, ADAPTIVE CONTROL AND EXTENDED SYNCHRONIZATION OF HYPERCHAOTIC SYSTE...ijccmsjournal
This work studies the dynamics, control and synchronization of hyperchaotic Lorenz-stenflo system and its
application to secure communication. The proposed designed nonlinear feedback controller control and
globally synchronizes two identical Lorenz-stenflo hyperchaotic systems evolving from different initial
conditions with unknown parameters. Adaptive synchronization results were further applied to secure
communication. The numerical simulation results were presented to verify the effectiveness of the designed
nonlinear controller and its success in secure communication application.
Output Regulation of SPROTT-F Chaotic System by State Feedback ControlAlessioAmedeo
This paper solves the output regulation problem of Sprott-F chaotic system, which is one of the classical chaotic systems discovered by J.C. Sprott (1994). Explicitly, for the constant tracking problem, new state feedback control laws have been derived for regulating the output of the Sprott-F chaotic system. Our controller design has been carried out using the regulator equations of C.I. Byrnes and A. Isidori (1990). The output regulation of the Sprott-F chaotic system has important applications in many areas of Science and Engineering. Numerical simulations are shown to illustrate the effectiveness of the control schemes proposed in this paper for the output regulation of the Sprott-F chaotic system.
An optimal control for complete synchronization of 4D Rabinovich hyperchaotic...TELKOMNIKA JOURNAL
This paper derives new results for the complete synchronization of 4D
identical Rabinovich hyperchaotic systems by using two strategies: active
and nonlinear control. Nonlinear control strategy is considered as one
of the powerful tool for controlling the dynamical systems. The stabilization
results of error dynamics systems are established based on Lyapunov second
method. Control is designed via the relevant variables of drive and response
systems. In comparison with previous strategies, the current controller
(nonlinear control) focuses on convergence speed and the minimum limits
of relevant variables. Better performance is to achieve full synchronization
by designing the control with fewer terms. The proposed control has
certain significance for reducing the time and complexity for strategy
implementation.
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ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF LÜ-LIKE ATTRACTORijcseit
This paper derives new results for the adaptive chaos stabilization and synchronization of Lü-like attractor
with unknown parameters. The Lü-like attractor is one of the recently discovered 3-scroll chaotic systems,
which was proposed by D. Li (2007). First, adaptive control laws are determined to stabilize the Lü-like
attractor to its unstable equilibrium at the origin. These adaptive laws are established using Lyapunov
stability theory. Then adaptive synchronization laws are determined so as to achieve global chaos
synchronization of identical Lü-like attractors with unknown parameters. Numerical simulations are
presented to validate and demonstrate the effectiveness of the proposed adaptive control and
synchronization schemes for the Lü-like attractor.
GLOBAL CHAOS SYNCHRONIZATION OF HYPERCHAOTIC QI AND HYPERCHAOTIC JHA SYSTEMS ...ijistjournal
This paper derives new results for the global chaos synchronization of identical hyperchaotic Qi systems (2008), identical hyperchaotic Jha systems (2007) and non-identical hyperchaotic Qi and Jha systems. Active nonlinear control is the method adopted to achieve the complete synchronization of the identical and different hyperchaotic Qi and Jha systems. Our stability results derived in this paper are established using Lyapunov stability theory. Numerical simulations are shown to validate and illustrate the effectiveness of the synchronization results derived in this paper.
THE DESIGN OF ADAPTIVE CONTROLLER AND SYNCHRONIZER FOR QI-CHEN SYSTEM WITH UN...IJCSEA Journal
This paper investigates the design problem of adaptive controller and synchronizer for the Qi-Chen system (2005), when the system parameters are unknown. First, we build an adaptive controller to stabilize the QiChen chaotic system to its unstable equilibrium at the origin. Then we build an adaptive synchronizer to achieve global chaos synchronization of the identical Qi-Chen chaotic systems with unknown parameters. The results derived for adaptive stabilization and adaptive synchronization for the Qi-Chen chaotic system are established using adaptive control theory and Lyapunov stability theory. Numerical simulations have been shown to demonstrate the effectiveness of the adaptive control and synchronization schemes derived in this paper for the Qi-Chen chaotic system.
ADAPTIVE CONTROL AND SYNCHRONIZATION OF LIU’S FOUR-WING CHAOTIC SYSTEM WITH C...IJCSEA Journal
This paper investigates the adaptive chaos control and synchronization of Liu’s four-wing chaotic system with cubic nonlinearity (Liu, 2009) and unknown parameters. First, we design adaptive control laws to stabilize the Liu’s four-wing chaotic system with cubic nonlinearity to its unstable equilibrium at the origin based on the adaptive control theory and Lyapunov stability theory. Next, we derive adaptive control laws to achieve global chaos synchronization of identical Liu’s four-wing chaotic systems with cubic nonlinearity and unknown parameters. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive chaos control and synchronization schemes.
Adaptive Controller Design For The Synchronization Of Moore-Spiegel And Act S...ijcsa
In this paper, we design adaptive controllers for the global chaos synchronization of identical MooreSpiegel systems (1966), identical ACT systems (1981) and non-identical Moore-Spiegel and ACT chaotic systems with unknown parameters. Our adaptive synchronization results derived in this paper for
uncertain Moore-Spiegel and ACT systems are established using Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the adaptive control method is very effective and convenient to synchronize identical and non-identical uncertain Moore-Spiegel and ACT chaotic
systems. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive synchronization schemes for the global chaos synchronization of the uncertain chaotic systems derived in this paper.
Adaptive Projective Lag Synchronization of T and Lu Chaotic Systems IJECEIAES
In this paper, the synchronization problem of T chaotic system and Lu chaotic system is studied. The parameter of the drive T chaotic system is considered unknown. An adaptive projective lag control method and also parameter estimation law are designed to achieve chaos synchronization problem between two chaotic systems. Then Lyapunov stability theorem is utilized to prove the validity of the proposed control method. After that, some numerical simulations are performed to assess the performance of the proposed method. The results show high accuracy of the proposed method in control and synchronization of chaotic systems.
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC BAO AND HYPERCHAOTIC XU SYSTEMS VIA ACTI...IJCSEIT Journal
This paper investigates the anti-synchronization of identical hyperchaotic Bao systems (Bao and Liu,
2008), identical hyperchaotic Xu systems (Xu, Cai and Zheng, 2009) and non-identical hyperchaotic Bao
and hyperchaotic Xu systems. Active nonlinear control has been deployed for the anti- synchronization of
the hyperchaotic systems addressed in this paper and the main results have been established using
Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the active
nonlinear control method is very effective and convenient to achieve anti-synchronization of identical and
non-identical hyperchaotic Bao and hyperchaotic Xu systems. Numerical simulations have been provided to
validate and demonstrate the effectiveness of the anti-synchronization results for the hyperchaotic Cao and
hyperchaotic Xu systems.
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC PANG AND HYPERCHAOTIC WANG-CHEN SYSTEMS ...ijctcm
Hyperchaotic systems are chaotic systems having more than one positive Lyapunov exponent and they have
important applications in secure data transmission and communication. This paper applies active control
method for the synchronization of identical and different hyperchaotic Pang systems (2011) and
hyperchaotic Wang-Chen systems (2008). Main results are proved with the stability theorems of Lypuanov
stability theory and numerical simulations are plotted using MATLAB to show the synchronization of
hyperchaotic systems addressed in this paper.
ACTIVE CONTROLLER DESIGN FOR THE OUTPUT REGULATION OF THE WANG-CHEN-YUAN SYSTEMecij
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GLOBAL CHAOS SYNCHRONIZATION OF HYPERCHAOTIC QI AND HYPERCHAOTIC JHA SYSTEMS ...ijistjournal
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Adaptive Control and Synchronization of Hyperchaotic Cai Systemijctcm
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GLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN LORENZ-STENFLO AND QI 4-D CHAOTIC S...ijistjournal
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Adaptive Stabilization and Synchronization of Hyperchaotic QI SystemCSEIJJournal
The hyperchaotic Qi system (Chen, Yang, Qi and Yuan, 2007) is one of the important models of four-
dimensional hyperchaotic systems. This paper investigates the adaptive stabilization and synchronization
of hyperchaotic Qi system with unknown parameters. First, adaptive control laws are designed to
stabilize the hyperchaotic Qi system to its equilibrium point at the origin based on the adaptive control
theory and Lyapunov stability theory. Then adaptive control laws are derived to achieve global chaos
synchronization of identical hyperchaotic Qi systems with unknown parameters. Numerical simulations
are shown to demonstrate the effectiveness of the proposed adaptive stabilization and synchronization
schemes.
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF HYPERCHAOTIC QI SYSTEM cseij
The hyperchaotic Qi system (Chen, Yang, Qi and Yuan, 2007) is one of the important models of fourdimensional hyperchaotic systems. This paper investigates the adaptive stabilization and synchronization of hyperchaotic Qi system with unknown parameters. First, adaptive control laws are designed to stabilize the hyperchaotic Qi system to its equilibrium point at the origin based on the adaptive control theory and Lyapunov stability theory. Then adaptive control laws are derived to achieve global chaos synchronization of identical hyperchaotic Qi systems with unknown parameters. Numerical simulations are shown to demonstrate the effectiveness of the proposed adaptive stabilization and synchronization schemes.
Sliding Mode Controller Design for Hybrid Synchronization of Hyperchaotic Che...ijcsa
This paper derives new results for the design of sliding mode controller for the hybrid synchronization of identical hyperchaotic Chen systems (Jia, Dai and Hui, 2010). The synchronizer results derived in this paper for the hybrid synchronization of identical hyperchaotic Chen systems are established using Lyapunov stability theory. Since the Lyapunov exponents are not required for these calculations, the sliding mode control method is very effective and convenient to achieve hybrid synchronization of the
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This paper presents synchronization of a new autonomous hyperchaotic system. The generalized
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This paper presents synchronization of a new autonomous hyperchaotic system. The generalized backstepping technique is applied to achieve hyperchaos synchronization for the two new hyperchaotic systems. Generalized backstepping method is similarity to backstepping. Backstepping method is used only to strictly feedback systems but generalized backstepping method expands this class. Numerical simulations are presented to demonstrate the effectiveness of the synchronization schemes.
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backstepping technique is applied to achieve hyperchaos synchronization for the two new hyperchaotic systems. Generalized back-stepping method is similarity to backstepping. Backstepping method is used only
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THE ACTIVE CONTROLLER DESIGN FOR ACHIEVING GENERALIZED PROJECTIVE SYNCHRONIZA...ijait
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hyperchaotic systems addressed in this paper. Numerical simulations are provided to illustrate the effectiveness of the GPS synchronization results derived in this paper.
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ANTI-SYNCHRONIZATION OF HYPERCHAOTIC WANG AND HYPERCHAOTIC LI SYSTEMS WITH UNKNOWN PARAMETERS VIA ADAPTIVE CONTROL
1. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
DOI : 10.5121/ijcseit.2013.3203 31
ANTI-SYNCHRONIZATION OF HYPERCHAOTIC
WANG AND HYPERCHAOTIC LI SYSTEMS WITH
UNKNOWN PARAMETERS VIA ADAPTIVE CONTROL
Sundarapandian Vaidyanathan1
1
Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University
Avadi, Chennai-600 062, Tamil Nadu, INDIA
sundarvtu@gmail.com
ABSTRACT
In chaos theory, the problem anti-synchronization of chaotic systems deals with a pair of chaotic systems
called drive and response systems. In this problem, the design goal is to drive the sum of their respective
states to zero asymptotically. This problem gets even more complicated and requires special attention when
the parameters of the drive and response systems are unknown. This paper uses adaptive control theory
and Lyapunov stability theory to derive new results for the anti-synchronization of hyperchaotic Wang
system (2008) and hyperchaotic Li system (2005) with uncertain parameters. Hyperchaotic systems are
nonlinear dynamical systems exhibiting chaotic behaviour with two or more positive Lyapunov exponents.
The hyperchaotic systems have applications in areas like oscillators, lasers, neural networks, encryption,
secure transmission and secure communication. The main results derived in this paper are validated and
demonstrated with MATLAB simulations.
KEYWORDS
Hyperchaos, Hyperchaotic Systems, Adaptive Control, Anti-Synchronization.
1. INTRODUCTION
Hyperchaotic systems are typically defined as nonlinear chaotic systems having two or more
positive Lyapunov exponents. They are applicable in several areas like lasers [1], chemical
reactions [2], neural networks [3], oscillators [4], data encryption [5], secure communication [6-
8], etc.
In chaos theory, the anti-synchronization problem deals with a pair of chaotic systems called the
drive and response systems, where the design goal is to render the respective states to be same in
magnitude, but opposite in sign, or in other words, to drive the sum of the respective states to zero
asymptotically [9].
There are several methods available in the literature to tackle the problem of synchronization and
anti-synchronization of chaotic systems like active control method [10-12], adaptive control
method [13-15], backstepping method [16-19], sliding control method [20-22] etc.
This paper derives new results for the adaptive controller design for the anti-synchronization of
hyperchaotic Wang systems ([23], 2008) and hyperchaotic Li systems ([24], 2005) with unknown
parameters. Lyapunov stability theory [25] has been applied to prove the main results of this
paper. Numerical simulations have been shown using MATLAB to illustrate the results.
2. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
32
2. THE PROBLEM OF ANTI-SYNCHRONIZATION OF CHAOTIC SYSTEMS
In chaos synchronization problem, the drive system is described by the chaotic dynamics
( )x Ax f x= + (1)
where A is the n n× matrix of the system parameters and : n n
f →R R is the nonlinear part.
Also, the response system is described by the chaotic dynamics
( )y By g y u= + + (2)
where B is the n n× matrix of the system parameters, : n n
g →R R is the nonlinear part and
n
u ∈R is the active controller to be designed.
For the pair of chaotic systems (1) and (2), the design goal of the anti-synchronization problem is
to construct a feedback controller ,u which anti-synchronizes their states for all (0), (0) .n
x y ∈R
The anti-synchronization error is defined as
,e y x= + (3)
The error dynamics is obtained as
( ) ( )e By Ax g y f x u= + + + + (4)
The design goal is to find a feedback controller uso that
lim ( ) 0
t
e t
→∞
= for all (0)e ∈Rn
(5)
Using the matrix method, we consider a candidate Lyapunov function
( ) ,T
V e e Pe= (6)
where P is a positive definite matrix.
It is noted that : n
V →R R is a positive definite function.
If we find a feedback controller u so that
( ) ,T
V e e Qe= − (7)
where Q is a positive definite matrix, then : n
V → R R is a negative definite function.
Thus, by Lyapunov stability theory [26], the error dynamics (4) is globally exponentially stable.
When the system parameters in (1) and (2) are unknown, we apply adaptive control theory to
construct a parameter update law for determining the estimates of the unknown parameters.
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3. HYPERCHAOTIC WANG AND HYPERCHAOTIC LI SYSTEMS
The hyperchaotic Wang system ([23], 2008) is given by
1 2 1 2 3
2 1 1 3 2 4
3 3 1 2
4 4 1 3
( )
0.5
0.5
x a x x x x
x cx x x x x
x dx x x
x bx x x
= − +
= − − −
= − +
= +
(8)
where , , ,a b c d are constant, positive parameters of the system.
The Wang system (8) depicts a hyperchaotic attractor for the parametric values
40, 1.7, 88, 3a b c d= = = = (9)
The Lyapunov exponents of the system (8) are determined as
1 2 3 43.2553, 1.4252, 0, 46.9794 = = = = − (10)
Since there are two positive Lyapunov exponents in (10), the Wang system (8) is hyperchaotic for
the parametric values (9).
Figure 1 shows the phase portrait of the hyperchaotic Wang system.
The hyperchaotic Li system ([24], 2005) is given by
1 2 1 4
2 1 1 3 2
3 3 1 2
4 2 3 4
( )x x x x
x x x x x
x x x x
x x x rx
= − +
= − +
= − +
= +
(11)
where , , , ,r are constant, positive parameters of the system.
The Li system (11) depicts a hyperchaotic attractor for the parametric values
35, 3, 12, 7, 0.58r = = = = = (12)
The Lyapunov exponents of the system (11) for the parametric values in (12) are
1 2 3 40.5011, 0.1858, 0, 26.1010 = = = = − (13)
Since there are two positive Lyapunov exponents in (13), the Li system (11) is hyperchaotic for
the parametric values (12). Figure 2 shows the phase portrait of the hyperchaotic Li system.
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34
Figure 1. Hyperchaotic Attractor of the Hyperchaotic Wang System
Figure 2. Hyperchaotic Attractor of the Hyperchaotic Li System
4. ANTI-SYNCHRONIZATION OF HYPERCHAOTIC WANG SYSTEMS VIA
ADAPTIVE CONTROL
In this section, we derive new results for designing a controller for the anti-synchronization of
identical hyperchaotic Wang systems (2008) with unknown parameters via adaptive control.
The drive system is the hyperchaotic Wang dynamics given by
5. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
35
1 2 1 2 3
2 1 1 3 2 4
3 3 1 2
4 4 1 3
( )
0.5
0.5
x a x x x x
x cx x x x x
x dx x x
x bx x x
= − +
= − − −
= − +
= +
(14)
where , , ,a b c d are unknown parameters of the system and 4
x∈ R is the state.
The response system is the controlled hyperchaotic Wang dynamics given by
1 2 1 2 3 1
2 1 1 3 2 4 2
3 3 1 2 3
4 4 1 3 4
( )
0.5
0.5
y a y y y y u
y cy y y y y u
y dy y y u
y by y y u
= − + +
= − − − +
= − + +
= + +
(15)
where 4
y ∈ R is the state and 1 2 3 4, , ,u u u u are the adaptive controllers to be designed.
For the anti-synchronization, the error e is defined as
1 1 1 2 2 2 3 3 3 4 4 4, , ,e e e ey x y x y x y x= + = + = + = + (16)
Then we derive the error dynamics as
1 2 1 2 3 2 3 1
2 1 2 4 1 3 1 3 2
3 3 1 2 1 2 3
4 4 1 3 1 3 4
( )
0.5
0.5( )
e a e e y y x x u
e ce e e y y x x u
e de y y x x u
e be y y x x u
= − + + +
= − − − − +
= − + + +
= + + +
(17)
The adaptive controller to solve the anti-synchronization problem is taken as
1 2 1 2 3 2 3 1 1
2 1 2 4 1 3 1 3 2 2
3 3 1 2 1 2 3 3
4 4 1 3 1 3 4 4
ˆ( )( )
ˆ( ) 0.5
ˆ( )
ˆ( ) 0.5( )
u a t e e y y x x k e
u c t e e e y y x x k e
u d t e y y x x k e
u b t e y y x x k e
= − − − − −
= − + + + + −
= − − −
= − − + −
(18)
In Eq. (18), , ( 1,2,3,4)ik i = are positive gains and ˆ ˆˆ ˆ( ), ( ), ( ), ( )a t b t c t d t are estimates for the
unknown parameters , , ,a b c d respectively.
By the substitution of (18) into (17), the error dynamics is obtained as
1 2 1 1 1
2 1 2 2
3 3 3 3
4 4 4 4
ˆ( ( ))( )
ˆ( ( ))
ˆ( ( ))
ˆ( ( ))
e a a t e e k e
e c c t e k e
e d d t e k e
e b b t e k e
= − − −
= − −
= − − −
= − −
(19)
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36
Next, we define the parameter estimation errors as
ˆ ˆˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )a b c de t a a t e t b b t e t c c t e t d d t= − = − = − = − (20)
Upon differentiation, we get
ˆ ˆˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )a b c de t a t e t b t e t c t e t d t= − = − = − = −
(21)
Substituting (20) into the error dynamics (19), we obtain
1 2 1 1 1
2 1 2 2
3 3 3 3
4 4 4 4
( )a
c
d
b
e e e e k e
e e e k e
e e e k e
e e e k e
= − −
= −
= − −
= −
(22)
We consider the candidate Lyapunov function
( )2 2 2 2 2 2 2 2
1 2 3 4
1
2
a b c dV e e e e e e e e= + + + + + + + (23)
Differentiating (23) along the dynamics (21) and (22), we obtain
( )
( ) ( )
2 2 2 2 2
1 1 2 2 3 3 4 4 1 2 1 4
2
1 2 3
ˆˆ( )
ˆˆ
a b
c d
V k e k e k e k e e e e e a e e b
e e e c e e d
= − − − − + − − + −
+ − + − −
(24)
In view of (24), we choose the following parameter update law:
1 2 1 5
2
4 6
1 2 7
2
3 8
ˆ ( )
ˆ
ˆ
ˆ
a
b
c
d
a e e e k e
b e k e
c e e k e
d e k e
= − +
= +
= +
= − +
(25)
Next, we prove the following main result of this section.
Theorem 4.1 The adaptive control law defined by Eq. (18) along with the parameter update law
defined by Eq. (25), where ,( 1,2, ,8)ik i = are positive constants, render global and exponential
anti-synchronization of the identical hyperchaotic Wang systems (14) and (15) with unknown
parameters for all initial conditions 4
(0), (0) .x y ∈ R In addition, the parameter estimation errors
( ), ( ), ( ), ( )a b c de t e t e t e t globally and exponentially converge to zero for all initial conditions.
7. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
37
Proof. The proof is via Lyapunov stability theory [25] by taking V defined by Eq. (23) as the
candidate Lyapunov function. Substituting the parameter update law (25) into (24), we get
2 2 2 2 2 2 2 2
1 1 2 2 3 3 4 4 5 6 7 8( ) a b c dV e k e k ek e k e k e k e k e k e= − −− − − − − − (26)
which is a negative definite function on
8
.R This completes the proof.
Next, we demonstrate our adaptive anti-synchronization results with MATLAB simulations. The
classical fourth order R-K method with time-step 8
10h −
= has been used to solve the hyperchaotic
Wang systems (14) and (15) with the adaptive controller defined by (18) and parameter update
law defined by (25).
The feedback gains in the adaptive controller (18) are taken as 5, ( 1, ,8).ik i= =
The parameters of the hyperchaotic Wang systems are taken as in the hyperchaotic case, i.e.
40, 1.7, 88, 3a b c d= = = =
For simulations, the initial conditions of the drive system (14) are taken as
1 2 3 4(0) 37, (0) 16, (0) 14, (0) 11x x x x= = − = =
Also, the initial conditions of the response system (15) are taken as
1 2 3 4(0) 21, (0) 32, (0) 28, (0) 8y y y y= = = − = −
Also, the initial conditions of the parameter estimates are taken as
ˆ ˆˆ ˆ(0) 12, (0) 4, (0) 6, (0) 5a b c d= = = − =
Figure 3 depicts the anti-synchronization of the identical hyperchaotic Wang systems.
Figure 4 depicts the time-history of the anti-synchronization errors 1 2 3 4, , , .e e e e
Figure 5 depicts the time-history of the parameter estimation errors , , , .a b c de e e e
8. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
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Figure 3. Anti-Synchronization of Identical Hyperchaotic Wang Systems
Figure 4. Time-History of the Anti-Synchronization Errors 1 2 3 4, , ,e e e e
9. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
39
Figure 5. Time-History of the Parameter Estimation Errors , , ,a b c de e e e
5. ANTI-SYNCHRONIZATION OF HYPERCHAOTIC LI SYSTEMS VIA ADAPTIVE
CONTROL
In this section, we derive new results for designing a controller for the anti-synchronization of
identical hyperchaotic Li systems (2005) with unknown parameters via adaptive control.
The drive system is the hyperchaotic Li dynamics given by
1 2 1 4
2 1 1 3 2
3 3 1 2
4 2 3 4
( )x x x x
x x x x x
x x x x
x x x rx
= − +
= − +
= − +
= +
(27)
where , , , , r are unknown parameters of the system and 4
x∈ R is the state.
The response system is the controlled hyperchaotic Li dynamics given by
1 2 1 4 1
2 1 1 3 2 2
3 3 1 2 3
4 2 3 4 4
( )y y y y u
y y y y y u
y y y y u
y y y ry u
= − + +
= − + +
= − + +
= + +
(28)
where 4
y ∈ R is the state and 1 2 3 4, , ,u u u u are the adaptive controllers to be designed.
For the anti-synchronization, the error e is defined as
1 1 1 2 2 2 3 3 3 4 4 4, , ,e e e ey x y x y x y x= + = + = + = + (29)
10. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
40
Then we derive the error dynamics as
1 2 1 4 1
2 1 2 1 3 1 3 2
3 3 1 2 1 2 3
4 4 2 3 2 3 4
( )e e e e u
e e e y y x x u
e e y y x x u
e re y y x x u
= − + +
= + − − +
= − + + +
= + + +
(30)
The adaptive controller to solve the anti-synchronization problem is taken as
1 2 1 4 1 1
2 1 2 1 3 1 3 2 2
3 3 1 2 1 2 3 3
4 4 2 3 2 3 4 4
ˆ( )( )
ˆ ˆ( ) ( )
ˆ( )
ˆ( )
u t e e e k e
u t e t e y y x x k e
u t e y y x x k e
u r t e y y x x k e
= − − − −
= − − + + −
= − − −
= − − − −
(31)
In Eq. (31), , ( 1,2,3,4)ik i = are positive gains and ˆ ˆˆ ˆ ˆ( ), ( ), ( ), ( ), ( )t t t t r t are estimates for
the unknown parameters , , , , r respectively.
By the substitution of (31) into (30), the error dynamics is obtained as
1 2 1 1 1
2 1 2 2 2
3 3 3 3
4 4 4 4
ˆ( ( ))( )
ˆ ˆ( ( )) ( ( ))
ˆ( ( ))
ˆ( ( ))
e t e e k e
e t e t e k e
e t e k e
e r r t e k e
= − − −
= − + − −
= − − −
= − −
(32)
Next, we define the parameter estimation errors as
ˆ ˆˆ ˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )re t t e t t e t t e t t e t r r t = − = − = − = − = − (33)
Upon differentiation, we get
ˆ ˆˆ ˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )re t t e t t e t t e t t e t r t = − = − = − = − = −
(34)
Substituting (33) into the error dynamics (32), we obtain
1 2 1 1 1
2 1 2 2 2
3 3 3 3
4 4 4 4
( )
r
e e e e k e
e e e e e k e
e e e k e
e e e k e
= − −
= + −
= − −
= −
(35)
We consider the candidate Lyapunov function
11. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
41
( )2 2 2 2 2 2 2 2 2
1 2 3 4
1
2
rV e e e e e e e e e = + + + + + + + + (36)
Differentiating (36) along the dynamics (34) and (35), we obtain
( )
( ) ( ) ( )
2 2 2 2 2
1 1 2 2 3 3 4 4 1 2 1 3
2 2
2 1 2 4
ˆˆ( )
ˆˆ ˆr
V k e k e k e k e e e e e e e
e e e e e e e r
= − − − − + − − + − −
+ − + − + −
(37)
In view of (37), we choose the following parameter update law:
1 2 1 5
2
3 6
2
2 7
1 2 8
2
4 9
ˆ ( )
ˆ
ˆ
ˆ
ˆ
a
r
e e e k e
e k e
e k e
e e k e
r e k e
= − +
= − +
= +
= +
= +
(38)
Next, we prove the following main result of this section.
Theorem 5.1 The adaptive control law defined by Eq. (31) along with the parameter update law
defined by Eq. (38), where ,( 1,2, ,9)ik i = are positive constants, render global and exponential
anti-synchronization of the identical hyperchaotic Li systems (27) and (28) with unknown
parameters for all initial conditions 4
(0), (0) .x y ∈ R In addition, the parameter estimation errors
( ), ( ), ( ), ( ), ( )re t e t e t e t e t globally and exponentially converge to zero for all initial
conditions.
Proof. The proof is via Lyapunov stability theory [25] by taking V defined by Eq. (36) as the
candidate Lyapunov function. Substituting the parameter update law (38) into (37), we get
2 2 2 2 2 2 2 2 2
1 1 2 2 3 3 4 4 5 6 7 8 9( ) rV e k e k ek e k e k e k e k e k e k e = − −− − − − − − − (39)
which is a negative definite function on
9
.R This completes the proof.
Next, we demonstrate our adaptive anti-synchronization results with MATLAB simulations. The
classical fourth order R-K method with time-step 8
10h −
= has been used to solve the hyperchaotic
Li systems (27) and (28) with the adaptive controller defined by (31) and parameter update law
defined by (38). The feedback gains in the adaptive controller (31) are taken as
5, ( 1, ,9).ik i= =
The parameters of the hyperchaotic Li systems are taken as in the hyperchaotic case, i.e.
35, 3, 12, 7, 0.58r = = = = =
For simulations, the initial conditions of the drive system (27) are taken as
12. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
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1 2 3 4(0) 7, (0) 26, (0) 12, (0) 14x x x x= = − = =
Also, the initial conditions of the response system (28) are taken as
1 2 3 4(0) 21, (0) 28, (0) 18, (0) 29y y y y= − = = − =
Also, the initial conditions of the parameter estimates are taken as
ˆ ˆˆ ˆ ˆ(0) 7, (0) 15, (0) 5, (0) 4, (0) 3r = = = = = −
Figure 6 depicts the anti-synchronization of the identical hyperchaotic Li systems.
Figure 7 depicts the time-history of the anti-synchronization errors 1 2 3 4, , , .e e e e
Figure 8 depicts the time-history of the parameter estimation errors , , , , .re e e e e
Figure 6. Anti-Synchronization of Identical Hyperchaotic Li Systems
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43
Figure 7. Time-History of the Anti-Synchronization Errors 1 2 3 4, , ,e e e e
Figure 8. Time-History of the Parameter Estimation Errors , , , , re e e e e
6.ANTI-SYNCHRONIZATION OF HYPERCHAOTIC WANG AND
HYPERCHAOTIC LI SYSTEMS VIA ADAPTIVE CONTROL
In this section, we derive new results for designing a controller for the anti-synchronization of
non-identical hyperchaotic Wang system (2009) and hyperchaotic Li system (2005) with
unknown parameters via adaptive control.
The drive system is the hyperchaotic Wang dynamics given by
14. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
44
1 2 1 2 3
2 1 1 3 2 4
3 3 1 2
4 4 1 3
( )
0.5
0.5
x a x x x x
x cx x x x x
x dx x x
x bx x x
= − +
= − − −
= − +
= +
(40)
where , , ,a b c d are unknown parameters of the system and 4
x ∈ R is the state.
The response system is the controlled hyperchaotic Li dynamics given by
1 2 1 4 1
2 1 1 3 2 2
3 3 1 2 3
4 2 3 4 4
( )y y y y u
y y y y y u
y y y y u
y y y ry u
= − + +
= − + +
= − + +
= + +
(41)
where , , , , r are unknown parameters, 4
y ∈ R is the state and 1 2 3 4, , ,u u u u are the adaptive
controllers to be designed.
For the anti-synchronization, the error e is defined as
1 1 1 2 2 2 3 3 3 4 4 4, , ,e e e ey x y x y x y x= + = + = + = + (42)
Then we derive the error dynamics as
1 2 1 2 1 4 2 3 1
2 1 1 2 2 4 1 3 1 3 2
3 3 3 1 2 1 2 3
4 4 4 1 3 2 3 4
( ) ( )
0.5
0.5
e a x x y y y x x u
e cx y x y x x x y y u
e dx y y y x x u
e bx ry x x y y u
= − + − + + +
= + − + − − − +
= − − + + +
= + + + +
(43)
The adaptive controller to solve the anti-synchronization problem is taken as
1 2 1 2 1 4 2 3 1 1
2 1 1 2 2 4 1 3 1 3 2 2
3 3 3 1 2 1 2 3 3
4 4 4 1 3 2 3 4 4
ˆˆ( )( ) ( )( )
ˆ ˆˆ( ) ( ) ( ) 0.5
ˆ ˆ( ) ( )
ˆ ˆ( ) ( ) 0.5
u a t x x t y y y x x k e
u c t x t y x t y x x x y y k e
u d t x t y y y x x k e
u b t x r t y x x y y k e
= − − − − − − −
= − − + − + + + −
= + − − −
= − − − − −
(44)
In Eq. (44), , ( 1,2,3,4)ik i = are positive gains and ˆ( ),a t ˆ( ),b t ˆ( ),c t ˆ( ),d t ˆ( ),t ˆ( ),t ˆ( ),t
ˆ( ),t ˆ( )r t are estimates for the unknown parameters , , , , , , , ,a b c d r respectively.
By the substitution of (44) into (43), the error dynamics is obtained as
1 2 1 2 1 1 1
2 1 1 2 2 2
3 3 3 3 3
4 4 4 4 4
ˆˆ( ( ))( ) ( ( ))( )
ˆ ˆˆ( ( )) ( ( )) ( ( ))
ˆ ˆ( ( )) ( ( ))
ˆ ˆ( ( )) ( ( ))
e a a t x x t y y k e
e c c t x t y t y k e
e d d t x t y k e
e b b t x r r t y k e
= − − + − − −
= − + − + − −
= − − − − −
= − + − −
(45)
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Next, we define the parameter estimation errors as
ˆ ˆˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )
ˆ ˆˆ ˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )
a b c d
r
e t a a t e t b b t e t c c t e t d d t
e t t e t t e t t e t t e t r r t
= − = − = − = −
= − = − = − = − = −
(46)
Upon differentiation, we get
ˆ ˆˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )
ˆ ˆˆ ˆ ˆ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( ), ( ) ( )
a b c d
r
e t a t e t b t e t c t e t d t
e t t e t t e t t e t t e t r t
= − = − = − = −
= − = − = − = − = −
(47)
Substituting (46) into the error dynamics (45), we obtain
1 2 1 2 1 1 1
2 1 1 2 2 2
3 3 3 3 3
4 4 4 4 4
( ) ( )a
c
d
b r
e e x x e y y k e
e e x e y e y k e
e e x e y k e
e e x e y k e
= − + − −
= + + −
= − − −
= + −
(48)
We consider the candidate Lyapunov function
( )2 2 2 2 2 2 2 2 2 2 2 2 2
1 2 3 4
1
2
a b c d rV e e e e e e e e e e e e e = + + + + + + + + + + + + (49)
Differentiating (49) along the dynamics (47) and (48), we obtain
( ) ( )
( ) ( )
( ) ( ) ( )
2 2 2 2
1 1 2 2 3 3 4 4 1 2 1 4 4 2 1
3 3 1 2 1 3 3
2 2 2 1 4 4
ˆˆ ˆ( )
ˆ ˆˆ+ ( )
ˆˆ ˆ
a b c
d
r
V k e k e k e k e e e x x a e e x b e e x c
e e x d e e y y e e y
e e y e e y e e y r
= − − − − + − − + − + −
− − + − − + − −
+ − + − + −
(50)
In view of (50), we choose the following parameter update law:
1 2 1 5 1 2 1 9
4 4 6 3 3 10
2 1 7 2 2 11
3 3 8 2 1 12
ˆˆ ( ) , ( )
ˆ ˆ,
ˆˆ ,
ˆ ˆ,
a a
b
c
d
a e x x k e e y y k e
b e x k e e y k e
c e x k e e y k e
d e x k e e y k
= − + = − +
= + = − +
= + = +
= − + = +
4 4 13
ˆ r
e
r e y k e
= +
(51)
Next, we prove the following main result of this section.
16. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
46
Theorem 6.1 The adaptive control law defined by Eq. (44) along with the parameter update law
defined by Eq. (51), where ,( 1,2, ,13)ik i = are positive constants, render global and
exponential anti-synchronization of the non-identical hyperchaotic Wang system (40) and
hyperchaotic Li system (41) with unknown parameters for all initial conditions 4
(0), (0) .x y ∈ R
In addition, all the parameter estimation errors globally and exponentially converge to zero for all
initial conditions.
Proof. The proof is via Lyapunov stability theory [25] by taking V defined by Eq. (49) as the
candidate Lyapunov function. Substituting the parameter update law (51) into (50), we get
2 2 2 2 2 2 2 2
1 1 2 2 3 3 4 4 5 6 7 8
2 2 2 2 2
9 10 11 12 13
( ) a b c d
r
V e k e k e
k e
k e k e k e k e k e k e
k e k e k e k e
= − −
−
− − − − − −
− − − −
(52)
which is a negative definite function on
13
.R This completes the proof.
Next, we demonstrate our adaptive anti-synchronization results with MATLAB simulations. The
classical fourth order R-K method with time-step 8
10h −
= has been used to solve the hyperchaotic
systems (40) and (41) with the adaptive controller defined by (44) and parameter update law
defined by (51).
The feedback gains in the adaptive controller (44) are taken as 5, ( 1, ,13).ik i= =
The parameters of the hyperchaotic Wang and Li systems are taken as in the hyperchaotic case,
i.e.
40, 1.7, 88, 3, 35, 3, 12, 7, 0. 58a b c d r = = = = = = = = =
For simulations, the initial conditions of the drive system (40) are taken as
1 2 3 4(0) 12, (0) 34, (0) 31, (0) 14x x x x= = − = =
Also, the initial conditions of the response system (41) are taken as
1 2 3 4(0) 25, (0) 18, (0) 12, (0) 29y y y y= − = = − =
Also, the initial conditions of the parameter estimates are taken as
ˆ ˆˆ ˆ(0) 21, (0) 14, (0) 26, (0) 16
ˆ ˆˆ ˆ ˆ(0) 17, (0) 22 (0) 15, (0) 11, (0) 7
a b c d
r
= = = − =
= = − = = = −
Figure 9 depicts the anti-synchronization of the hyperchaotic Wang and hyperchaotic Li systems.
Figure 10 depicts the time-history of the anti-synchronization errors 1 2 3 4, , , .e e e e
Figure 11 depicts the time-history of the parameter estimation errors , , , .a b c de e e e
Figure 12 depicts the time-history of the parameter estimation errors , , , , .re e e e e
17. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
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Figure 9. Anti-Synchronization of Hyperchaotic Wang and Hyperchaotic Li Systems
Figure 10. Time-History of the Anti-Synchronization Errors 1 2 3 4, , ,e e e e
18. International Journal of Computer Science, Engineering and Information Technology (IJCSEIT), Vol.3, No.2,April2013
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Figure 11. Time-History of the Parameter Estimation Errors , , ,a b c de e e e
Figure 12. Time-History of the Parameter Estimation Errors , , , , re e e e e
7. CONCLUSIONS
This paper has used adaptive control theory and Lyapunov stability theory so as to solve the anti-
synchronization problem for the anti-synchronization of hyperchaotic Wang system (2008) and
hyperchaotic Li system (2005) with unknown parameters. Hyperchaotic systems are chaotic
systems with two or more positive Lyapunov exponents and they have viable applications like
chemical reactions, neural networks, secure communication, data encryption, neural networks,
etc. MATLAB simulations were depicted to illustrate the various adaptive anti-synchronization
results derived in this paper for the hyperchaotic Wang and Li systems.
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Author
Dr. V. Sundarapandian earned his D.Sc. in Electrical and Systems Engineering from
Washington University, St. Louis, USA in May 1996. He is Professor and Dean of the
R & D Centre at Vel Tech Dr. RR & Dr. SR Technical University, Chennai, Tamil
Nadu, India. So far, he has published over 300 research works in refereed
international journals. He has also published over 200 research papers in National and
International Conferences. He has delivered Key Note Addresses at many
International Conferences with IEEE and Springer Proceedings. He is an India Chair
of AIRCC. He is the Editor-in-Chief of the AIRCC Control Journals – International
Journal of Instrumentation and Control Systems, International Journal of Control
Theory and Computer Modeling, International Journal of Information Technology, Control and
Automation, International Journal of Chaos, Control, Modelling and Simulation, and International Journal
of Information Technology, Modeling and Computing. His research interests are Control Systems, Chaos
Theory, Soft Computing, Operations Research, Mathematical Modelling and Scientific Computing. He
has published four text-books and conducted many workshops on Scientific Computing, MATLAB and
SCILAB.